Electrical timing circuit



4 Sheets-Sheet 2 J. R. WILKERSON ELECTRICAL TIMING CIRCUIT Filed Feb. 28, 1 942 Feb. 22, 1944.

Feb. 2 2, 1944. J. R. wlLKl-:RsoN

ELECTRICAL TIMING CIRCUIT Filed Feb; 28, 1942 4 Sheets-Sheet 3 W WQ,

/N VEA/T0@ J. R. W/L KERS ON A 7' TORNE Y Feb. 22, 1944. J. R. wlLKERsoN 2,342,313

' ELECTRICAL TIMINC CIRCUIT Filed Feb. 28, 1942 4 Sheets-Sheet 4 kk 1km.

IH l mwo .ESSEC s! 5mm x Patented Feb. 22, 1944 UNITED STATES PATENT OFFICE ELECTRICAL 'rIMING CIRCUIT Jefrerson n. Wilkerson, Brooklyn, N. Y., assignmto Bell Telephone laboratories, Incorporated, New York, N. Y., a corporation of New York Application February 28, 1942, Serial No. 432,822

13 Claims.

This invention relates to eiectrical timingcircuits and, more particularly, to timing circuits used in start-stop telegraph systems for timing of operations therein.

It is an object of the invention to provide timing circuits of this kind which are more stable and accurate than those hitherto used.

Timing circuitsof this kind may be used in start-stop signaling systems of different types having the common requirement that operations in response to the individual pulses of an incoming signal must be accurately timed with respect to the incoming start pulse of the signals. Such timing circuits may thus be used in start-stop telegraph receivers and regenerative repeaters and in various types of test circuits used for the observation of operating conditions in the teletypewriter plant.

Different types of timing systems have been proposed in the past for this purpose.

Thus, it has been general practice to use a rotary start-stop distributor for determining the timed intervals. This type of device has certain disadvantages, when operated at high speed and where high accuracy of timing is desired, because the mechanical starting mechanism as well as the constantly running friction clutch used with this apparatus are subject to wear and, therefore, tend to variably affect the operation of the distributor, particularly at starting. Another disadvantage of this type of device, when used at high speed, is to be found in the fact that there is a certain minimum length of the distributor segments below which definite, well-formed timing impulses cannot be produced by the segments; this has been found to be particularly disadvantageous in certain testing systems for checking the operating conditions of the teletypewriter plant.

It has also been proposed to use a timing system without mechanical rotating parts but based on oscillating relay circuits or on oscillating circuits using gas-fllled tubes for the timing of the individual p..`ses and using similar oscillating relay or tube circuits, more slow acting, for stopping the pulse timing oscillator at the end of each signal train.

Reference` may be had to U. S. Patents 1,771,445, issued to Parker-vernam on July 29, 1930, and 2,154,623, issued to Kinkead on April 18, 1939, disclosing oscillating relay circuits of this kind; and 2,133,456, issued to Kinkead on October18, 1938, disclosing oscillating circuits using gas-filled tubes for timing purposes. Reference may also be had to U. S. Patent 2,132,678,

issued to Cowan October 1 1, 1938, disclosing a signal distortion measuring device for teletypewriter circuits which uses a rotating start-stop distributor for timing the operations of the measuring device.

With the steady demand for increased eillciency of the telegraph plant, the speed of telegraph operation has been greatly increased during the last few years and further increase in speed may be anticipated. It is therefore evident that a higher degree of accuracy of operation of commercial telegraph apparatus will be necessary. For purposes of checking the operations of such telegraph apparatus, testing systems of different types have been developed which operate on a start-stop basis and such testing systems must necessarily be accurate within very narrow limits, in order to be able to indicate small deviations from the ideal operation of the commercial apparatus.

It is therefore a principal object of the invention to provide a start-stop timing system which is highly accurate and dependable in operation, and whichl will require less maintenance than present timing systems using rotary distributors.

It is a more specific object to provide a testing system of the kind disclosed in the patent to Cowan, referred to above, but adapted for operation with a timing system of the type provided in accordance with the invention for the purpose of securing a higher degree of accuracy and of `enabling the testing system to measure a higher percentage of distortion. i

In accordance with a feature of the invehtion a timing circuit is provided which includes an impulse circuit for producing evenly spaced impulses definitely related to the start instant and an interrupter circuit which establishes a circuit condition for an extremely short interval in response to each of the evenly spaced impulses.

'The timing circuit thus establishes very short intervals at uniformly spaced reference instants definitely related to the start instant for controlling the operations in a telegraph system. More specifically the interruptor circuit includes a gas-filled tube which is red infresponse to each of the evenly spaced impulses and is extinguished by other circuit means after a definite brief interval, thereby` establishing a conducting condition in its output circuit during each brief interval.

In accordance with another features of the invention, an oscillatory circuit of the relaxation type is provided for restoring the said tim,- ing circuit to rest condition after the establish# ment of a predetermined number of said inter vals. This circuit includes a timing condenser for control of a vacuum tube, the condenser being charged and. discharged once for each series of operations. The arrangement is such that the control period by this circuit lies between points so located on the condenser voltage curve that the termination of the control period will be definitely limited.

Other objects and features of the invention will be apparent from the following detailed description of a specific testing system embodying the invention. It should, however, be understood that the various features of the invention may be incorporated in telegraph systems other than that described hereinafter, which is disclosed by way of example for the purpose of fully explaining the invention and its mode of operation as incorporated in a practical system.

In the following detailed description of the testing system and its operation reference will be made to the attached drawings, in which:

Figs. 1, 2 and 3, when properly placed with respect to each other in accordance with the diagram in Fig. 6, show the circuit arrangement;

Fig. 4 shows an alternative impulse producing circuit which may be substituted for the impulse producing circuit included in the system shown in Figs. 1, 2 and 3; and v Fig. 5 is a diagram showing the relative tim, ing of various operating conditions in the circuit.

As already stated above, the system in various respects is similar to that disclosed in the Cowan patent and is adapted to be used for the samepurposes,` namely, to determine the appearance of normal and abnormal conditions in start-stop telegraph circuits as they aect the start-stop signals in such circuit.

Reference may, therefore, be had to the Cowan patent for an explanation of the different types of distortion that may be observed in startstop signals by means of a testing system of the present type. The observations are made on two meters, Aas in the Cowan system, namely, the peak-.yoltmeter which gives steady indications of the maximumtotal distortion of any individual pulse, and the bias-meter which gives integrated indications of bias present in a plurality of successive pulses and which may be switched to indicate displacement of mark-tospace or space-to-mark transitions or average displacement of both.

Referring now to Figs. 1, 2 and 3 of the drawings, the system comprises a number of main portions as follows:

Thefinput circuit, shown in Fig. 1, whereby the set is connected, for example, to a commercial operating circuit and whereby the incoming signals are applied to the testing equipment.

The comparison circuit, shown in Fig. l, in which the incoming signals are received and caused to set up charges on a pair of unit condensers which in turn affect the two meters in accordance with their acquired charges once for each unit pulse of a series of pulses representlng a. character. bias-meter.

An impulse circuit, shown in Fig. 2, for establishing a series of uniformly separated reference instants, one for each unit pulse in a signal series. This includes the condenser timing circuit which conditions the unit condensers for each test. f

This circuit includes the.

accasie A character timing circuit, shown in Fig. 2, for stopping the impulse circuit at the end o acharacter series.

A start-stop relay circuit, shown in Fig. l, for starting the timing operations in response to an incoming start pulse and for restoring the system to normal in response to the stopping action of the character timing circuit.

The peak-voltmeter circuit showngn Fig. 3 and connected to the comparison circuit for giving an indication of the maximum distortion in the incoming signals during a convenienttime interval, and obtaining its power through suitable equipment from an alternating current source.

A power supply circuit, shown in Fig. 3, for supplying constant current and various potentials to the test system and obtaining its power through suitable equipment from an alternating current source.

The system, as shown in the drawings, is arranged for operation under a number of different conditions and for this reason includes a number of manual keys and neutral-type relays for adapting the diierent portions of the circuit to the spectic conditions existing in the commercial circuit which is to be tested. Thus, the circuit, as shown in the drawing, may be adapted to test signals using a 'Z1/2 unit code or an 81/2 unit code and it is apparent that it may be further adapted for a 7-unit code or other start-stop codes. The circuit, as shown, may also be adapted for diierent signaling speeds at the different codes. Thus, signals may be accurately tested having dot frequencies of 15, 23, or 28 cycles per second corresponding, for example, to 40, 60, and '75 words per minute for a code using 7l/2 units. The circuit is also adapted to test either neutral-type signals or polar signals.

A distortion measuring set of this type is usually permanentlyinstalled in a switchboard in the telegraph exchange and in that case' is made available for tests at the various operators positions by means of extension circuits and test set or abnormal conditions of the test set at the various operators positions. A circuit arrangement for such interconnection of operators positions for the use of a common distortion measuring set at any one position is disclosed in U. S.

Patent 2,244,566, issued June 3, 1941, to J. T.

Neiswinter, and it will be readily apparent to those skilled in the art how the input circuit shown in Fig. 1 of the present drawings may be incorporated in such an interconnecting system. It will be rst assumed that the measuring set is to bused for the observation of start-stop signals in a commercial circuit using the 71A; unit code at a dot frequency of about 23 cycles per second and using signals ofthe neutral type. with marking pulses represented by current condition and spacing pulsesA represented by no-current condition-in the line. Each cl-aracter will thus be represented by a series of pulses beginning with a spacing start pulse and ending with a marking stop pulse and having five selecting pulse intervals between the start and stop pulses. Thus, a signal series of pulses representing a character begins with a start transition from marking to spacing followed by transitions I, II, III, IV and V from marking to spacing and spacing rto marking at transition points 2, 3, 4 and 5, respectively, in accordance with the code, and ending with a stop transition from spacing to marking. In a commercial system the length of a stop pulse is 1.42 times the length of the unit pulse during continuous transmission. An example of such a signal series representing a character is shown diagrammatically in Fig. 5-A.

The signals impressed upon thetest circuit may be those passing between stations on a busy commercial circuit or they may be signals special- Jy transmitted over an idle commercial circuit. The traiiic need not be interrupted or otherwise disturbed by the tests.

The vcircuit is shown in the drawings as being in condition for operation with a line circuit of the assumed type and in rest condition, as during a stop interval.

Input circuit The incoming line circuit which may be connected in any desirable manner to a commercial circuit, is connected by the insertion of plug |02 into jack |03 to the line Vcircuit within the set; this circuit isI normally closed by normal contacts of relay |04. When the plug |02 is inserted the closing of contacts |03a of the jack causes the operation of relay |04 which, in operating, extends the line circuit to contacts of relay |05, where the line circuit remains closed through normal contacts of that relay.

A busy lamp |06 is now lighted over a circuit from battery through the lamp, make contact c of relay |04, conductor H3, break contacts of key 201 and break contacts of relay 20| to a ground applied from the interconnecting circuit, referred to above, for the operators positions in a manner of no importance for an understanding of the invention.

Relay is next operated from battery at make contacts e of relay |04 and thereby extends the incoming line circuit to the upper winding of polar relay |40. Relays |04 and |05 remain op-- erated until the plug |02 is removed from the jack |03 at the end of an observation.

Comparison circuit Relay |40 has a lower biasing winding normally tending to operate the relay to its spacing contact. When, as just described, the line circuit is extended to the upper winding of relay |40, marking current will flow in this winding during the stop condition, overcoming the biasing` winding and holding the relay operated to marking, thereby supplying plus battery to the grounded potentiometer |42 and also over a resistance |45 through the windings of polar relays |50 and |60 to the mid-point of potentiometer |46, which point is at ground potential. It will be noted that when the set is not in use there is a normal holding circuit from battery at jack |08 over break contact c of relay |05 through the upper winding of relay |40 and over break contact d to ground for holding relay |40 normally to marking as shown inthe drawings; when relay |05 1s operated, this holding circuit is opened and relay |40 is held in marking condition by the marking condition of the incoming line circuit. Under this condition relays |50 Aand |60 are held to marking and relays |40, |50 and |60 are in.condi tion to respond to the transitions of incoming pulses, relays |50 and |60 operating shortly after relay |40 to their marking and spacing contacts.

With the circuit in the condition shown, unit condensers |5| and |6| are connected over the marking contacts of relays and |60 simultaneously to two different circuits, respectively, and these connections are reversed when relays |50 and are operated to spacing. Condenser |66 is normally connected to the constant current supply circuit over marking contact of relay |60, constant current conductor 336:1, resistance 210, constant current conductor 336, meter 335 to the constant current supply circuit at the plate e of vacuum tube 330. As will be explained subsequently, the constant current supply circuit is arranged to deliver a substantially constant current into a varying impedance or voltage, such as that of a charging or discharging condenser, so that normally the condenser |6| will become charged over the traced circuit with a constant current irrespectively of its increasing potential. However, under the stop condition, condenser |6| is also connected over the marking contact of relay |10 and conductor 322 to adjustable point 32| of potentiometer 320. The potential applied from point 32| to condenser |6| remains xed and is called the stop-compensating voltage.

The other unit condenser |5| is normally connected over the marking contact of relay |50 to a reference potential, which circuit may be traced over the marking contact of relay |50,

over resistance |52 and condenser |53 connected,

in multiple by contact e of relay ||8, over contact d of relay H8, conductor 342a, resistance 34|, contact of key 343, primary winding of transformer 344, conductor 342 to point 348 of a potentiometer circuit from negative battery through resistance 341, the cathode plate circuit of vacuum tube 340 to ground. As will be explained subsequently, the reference potential at point 348 is maintained at a standard value which is used for comparison purposes in the tests to be described. Potentiometer 320 is so adjusted that the stop-compensating voltage at point 32| and the reference potential of point 348 will be equal during the stop condition. Thus. both unit condensers |5| and |6| are charged during the stop interval to a potential equal to the reference potential. The circuits for bias-meter |90 will be described below.

Peak-voltmeter circuit The left winding of transformer 344 has a grounded mid-point and is connected through rectifier vacuum tubes 35| and 352 for rectifica.- tion of current in both directions and for charging of condenser 36| over the circuit to ground at potentiometer 362. Under the rest condition of the system, as shown in the drawings, no current' flows in the transformer and condenser 36| remains uncharged; however, during test conditions when current flows in one or the other direction through the primary of transformer 344, condenser 36| will acquire -a charge which is applied to the grid of vacuum tube 360 for the peakvoltmeter 310. This meter is connected to the conjugate points of a Wheatstone bridge having the following arms: the first arm including resistance 363, cathode-plate circuit of tube 360, resistance 364; second arm, right side of potentiometer 365; third arm, left side of potentiometer 365; fourth arm, resistance 366. Direct current is applied to the supply points of the bridge circuit from the terminals 395 and 306 of a power supply equipment. With no charge on condenser 36| and a corresponding plate current in tube 360, the potentiometer 365 is adjusted to give zero current in the meter 310. The meter will then give an indication each time current flows through transformer 344 and causes condenser 36| to acquire a higher charge, and the deflection of the4 meter will be in proportion to the peak `current in the primary winding of the transformer 344. The key 343 serves to reverse the input to the peak-voltmeter current for checking the .sym-

Start-stop relay circuit During the stop condition the impulse circuit and the` character timing circuit are held inoperative by means of relay |00. Polar relays and |80 have lower biasing windings which are normally energized, the biasing winding of relay |10 normally operating the relay to marking, and

that of relay |80 tending to operate the relay to spacing. The circuit for the upper operating winding of relay |10 is open at the spacing contact of relay |80. The upper operating Winding of relay |80 'is normally energized from' plus,` potential on potentiometer |42 through the cathodeplate circuit of vacuum tube 220 in the character timing circuit. The operating winding, overcoming the biasing winding, holds relay |80 toA marking. When relay |40, in response to a spacing pulse, operates to its spacing contact, negative potential is applied from potentiometer |42 to the plate circuit of tube 220 rendering the tube 220 non-conducting; relay |80 then operates to spacing, thereby starting the character timing circuit and the impulse circuit upon a cycle of operations.

Character timing circuit The character timing circuit includes a set of timing condensers 222, 222a and 222b of which the iirst two normally are connected in multiple for use under the assumed conditions, namely, for a speed of 60 words per minute. Condensers 222 and 222a in multiple are normally charged from 4positive battery of 130 volts through resistance 22| to ground through the rectifier vacuum tube 225. Under this condition the upper plate of condenser 222 and the right-hand plate of condenser 222a, connected to point 228, will be at plus potential and the other plates, connected tol point 221, will be at ground potential, with a'. charge potential of 130 volts. Resistance 22| is comparatively low for quick charging of the condensers during the stop interval. With plus potential connected to the plate of rectifier 225, this tube will be in conducting condition; with the same potential applied to the grid and with positive potential applied to theplate of tube 220, this tube will be in conducting condition.

When the relay |80 operates to spacing in response to the operation of relay |40 to spacing, a comparatively low negative potential on the potentiometer IBi is applied over the spacing contact of relay |80 through the operating winding of relay I 10 to the upper point 226 at one side of condensers 222 and 222a. With a. potential of -20 volts applied in this manner to the point 226, the potential of point 221 will be -150 volts and both tubes 220 and 225 will be ren dered non-conductive. Under this condition,

condensers 222 and 222e will slowly discharge over a circuit from positive 130 volt battery through high resistance 223 to the negative potential on potentiometer li. This discharge condition will prevail until the charge on the condensers has been reversed and raised to a value at which the condenser potential is about volts, at which time the potential of point 221 will pass through zero and the tubes 220 and 225 will again'become conductive. With tube 220 in conducting condition and relay |40 in marking position, relay |80 will 'be operated back to its marking position, thereby removing the negative potential from the condensers at point 226, so that the condensers thereafter will be quickly charged from plus battery over resistance 22| and through the rectifier tube 225, thereby restoring the character timing-circuit to its original condition. The timing of the charging period for these condensers is such that they will be fully charged to 130 volts within a fraction of the stop interval and the timing of the discharging period of these condensers is such that, upon the discharge commencing immediately in response to a start transition, the

condensers will have acquired their reversed` charge of +20 volts for rendering the tubes 220 and 225 conductive, shortly after the normal arrival of the "stop transition. The charging cycle for condensers 222 andr222a is shown diagrammatically in Fig. 5-D, and the corresponding variation in the cathode-grid potential in tube 220 is shown in Fig. 5--E.

It will be noted that a very high discharging potential is used in this c lrcuit and that the effective point at which the timing period is terminated is only slightly past the middle point of the condenser voltage curve. Thus, the battery potential is 130 volts and the condenser potential is l30+20 or 150 volts at the moment the discharge commences; the total being 280 volts, which insures a steepvoltage characteristic. The charge reverses at .zero volts on the condenser and the current continues vuntil the condenser has a voltage of 20 volts in the opposite direction. Therefore, the timing period will be terminated at a point at which the rate of change of voltage with time is high. The time at Which the condenser reaches a charge corresponding to 20 volts in reverse direction thus will be sharply delimited and high accuracy of timing is thus secured.

This circuit has been found to operate satisfactorily with signals of the '1l/2 unit code at a speed of 23 cycles per second with the following circuit constants:

Resistance 22| '4,650 ohms Condenser 222 .4 microfarad Condenser 222m .l1 microfarad Resistance 223 385,000 ohms Resistance 224 500 ohms ica Type SHSG Plus battery through 2000 ohm resistance volts Impulse circuit The impulse circuit includes a double vacuum tube, which for the present purposes may be considered as two separate tubes, the righthand portion 230 being connected in the oscillatory circuit and the left-hand portion 240 operating as a detector in the output circuit o! the oscillatory circuit.

The Voscillatory circuit comprises the twowinding inductance coil 23| and the variable condenser 232, the lowerjunction point being grounded and the upper junction point being connected to the output circuit leading to the control grid oi? detector tube 240. The condenser 232 is normally connected to the upper junction' by the break contacts d of relay 202, but may be replaced by condenser 232a or by both the condensers 232a and 232D by operation of relays 202 and 204 for changing the frequency of oscillation, as will be further explained below.

The cathode-anode circuit of tube 230 includes a direct current source and resistance 231 and is connected across the lower winding of coil 23| tor compensation of the decrement of the oscillatory circuit. The control electrode is connected over the break contacts b of relay 202 to the adjustable point of potentiometer 233 which is bridged across the upper winding of coil 23| over break contact c of relay 202; by proper ad,- iustment of the potentiometer point the oscillatory circuit may have zero decrement and the amplitude of oscillation will remain substantially constant over a period of more than ten oscillations for a given adjustment. The potentiometer 233 may be replaced by the potentiometer 233e by operation of relay 202 when the circuit is to be used at another frequency, thereby obviating readjustment of the tube circuit each time the set is used at different operating frequencies in the line circuit.

The condenser 232 may be adjusted for oscillation at 45.6 cycles per second corresponding to an operating speed of 22.8 cycles per second or 60 words per minute for a 'I1/2 unit code. Thus the circuit maybe adjusted to produce exactly one cycle for each standard pulse period of the signals, thereby establishing a series of accurate comparison instants in the test set.

However, for start-stop operation it is essential that the comparison `instants be deflnitely related to the start instant during successive incoming pulse series and be uniformly spaced during each pulse series; it is therefore necessary that the oscillatory circuit be started andstopped for each' pulsecseries. Thus during the stopcondition the pulse circuit is held cocked, that is, it is prevented from oscillating by the application of a negative potential from the potentiometer DI over the marking contact of relay |00, conductor |62, resistance 236, break contact a of relay`202 and resistance 234 to the upper junction of the oscillatory circuit. A steady-state condition is thus established during which current flows through the windings of coil 23|, storing the energy of oscillation in the magnetic ilux of the coil, and during which' the charge on the condenser 232 is practically zero.-

Upon removal of the negative potential by ther operation of relay |80 in response to an incoming start transition the oscillatory circuit will be free to oscillate and the ilrst oscillation will be identical with subsequent oscillations and thus will have the same amplitude and waveshape.

' In this manner it is possible to accurately establish a comparison instant even during the tlrst cycle alter release from th steady state, since with zero decrement there will be no gradual building up of the amplitude as in the case of starting an oscillatory circuit intended for continuous operation.

When relay |00 is operated to again close its marking contact in response to an incoming stop transition, the oscillatory circuit will quickly return to its steady-state condition under the damping effect of resistances 234 and 236. 1 With the proper values of the negative potential at potentiometer |8| and of the resistances 234 and 236 i'or a given frequency, a current will flow in coil 23| during the stop condition which will establish a desired amplitude of oscillation, at the same time as the eiect of resistances 234 and 236 will be such as to return the circuit to the steady state in a critically damped manner, and well within the normal stop period Inasmuch' as it is important to accurately establish the iirst reference instant, it is essential that the rst cycle be started oil' without delay or distortion, as by transients or harmonics other than those that determine the regular wave shape of the oscillations. The importance of producing a sinusoidal wave shape, therefore, is apparent. Thus wh'en by design the circuit is incapable of producing other harmonics than the basic, the oscillations may be started without transients and will remain constant if adjusted for zero decrement.

The main'requirements for producing va Inusoidal wave form are, that the circuit must be simple and `must contain no other energy storing elements than the inductance coil and the condenser. ments are:

The output circuit should be purely resistive;

There must be no other capacitance th'an the condenser in the oscillatory circuit;

There must be no other linductance thany the windings of the coil in the oscillatory circuit;

The two windings of the coil should have a coemcient of coupling equal to unity;

The vacuum tube should be operated within the straight-line lportion of its characteristic; and

The ampliiication factor of the tube should be such that dissipation of energy is compensated for.

A circuit designed to answer these requirements may be held cocked by a current through coil 23| from theA dampingy circuit equal tothe oscillatory current at maximum amplitude. When the current supply is disconnected (by relay |00) the current in the coil will decay, following a cosine curve identical with that of the subsequent oscillations; at the Vsaine time the condenser voltage will ri'se from its steady state value of about zero volts, following a sine curve identical with that of the subsequent oscillations. Sincel the circuit by design is incapable of producing harmonics other than the basic, the first cycle will be free oi.' extraneous transients.

Forthe purposes of the invention the desired sinusoidal operation of this circuit may be secured with suillclent accuracy by the use of ap- Stated more specifically the require-l ready for a new series of oscillations every time a start pulse arrives. A series of voltage oscillations produced by the oscillatory circuit during a character series of pulses is shown diagrammatically in Fig. -F.

The following circuit constants for the impulse circuit have been found to give satisfactory operation at 22.8 cycles per second:

Inductance 23I 65 henries Condenser 232 .165 to .210 microfarad Potentiometer 233 4.5 megohms Resistance 234 3,600 ohms Resistance 236 4,900 ohms Resistance 231 1,000 ohms Equivalent resistance of potentiometer I3I 1,000 -ohms Potential at IBI -50 volts Plate battery +130 volts Vacuum tube 230-240, made by Radio Corporation of America--- Type 6F8G two-winding inductance 23|' and the variablev condenser 232', the lower junction point being grounded and the upper Junction point being connected to the output circuit.

The cathode-anode circuit of tube 230 includes a. direct current source and the lower winding of coll 23 I for feeding back to the oscillatory circuit under control of the control electrode or grid which is connected to the adjustable point of potentiometer 233' bridged across the oscillatory winding of coil 23|'.

The circuit may be adjusted to perform exactly like that in Fig. 2 though by different inherentoperations, and it may be cocked in the same manner by the application of a steady-state current from the potentiometer I 8i' over conductor |312 and .resistance 234' and through the oscillatory winding of coil 23| i The requirements listed above for the circuit :in Fig. 2 also hold for this circuit, which thus will include the main features of producing a sinusoidal Wave shape with substantially zero change of amplitude for at least twenty oscillations, and of starting after being cocked without extraneous transients, its performance being illustrated ln Fig. 5-F. This circuit thus is adapted to serve the purposes of the invention.

The detector tube 240 has its cathode-plate circuit connected'over the primary winding of trans former 24|, break contact a of relay 203, potentiometers 242 and 243 and break contact c of relay 203. The potentiometers 242 and 243 are connected across plus and minus batteries in series over break contacts b of relay 202 in such a manner that a positive potential may be supplied from potentiometer 242 to the plate and a lower potential from potentiometer 243 to the filament Vof tube 240. By adjustment of the potentiometer points individually, a desired potential difference `may be applied to the cathode-anode circuit in the tube and by echanically locking the two contact points toget er for simultaneous adjustment o! them this potential difference may be maintained at the same time as a proper potential relation with respect to the grid of the tube is established for orienting purposes. It should be underf stood that the two potentiometers may` be replaced by a single potentiometer with two adjustable points.

The control grid of tube 240 is connected to the upper Junction of the oscillatory circuit so that an oscillating voltage will be impressed thereon. For a given adjustment of potentiometers 242 and 243, the tube 240 will be non-conducting while the potential impressed upon the grid is below a predetermined value slightly negative relative to the cathode potential, and will be conducting when the potential on the grid is above this value. Thus. the tube will be conducting during the upper portions of each cycle of the oscillations. as indicated by the shaded portions in Fig. 5-F above the horizontal line f-.J, which represents the critical potential at which the condition in the tube changes. The correspondingv current pulses through the detector tube 240 and the primary winding of transformer 24I are shown diagramvmatically in Fig. 5--G. By proper'adjustment of the potentiometers 242 and 243 the critical potential and thus line f-f may be varied between the positive and negative maximum amplitudes of the Gil oscillations, thereby shifting the instant at which the detector tube 240 becomes non-conducting between the instants of the maximum and minimum amplitudes.

,Inthis manner. two voltage impulses will be generated in the secondary winding of transformer 24| during each cycle of the oscillations, namely. an impulse of relatively low maximum amplitude in a negative direction at the instant the detector tube 2 40 becomes conducting on the rising slope and an impulse of relatively high maximum amplitude in a positive direction at the instant the tube 240 becomes non-conductive on Y the descending slope. These impulses in the secondary winding of transformer 24I are schematically shown in Fig. 5H. The positive voltage pulses from the secondary of transformer 24| are impressed upon the grid of the gas-lled tube 250 to render this tube conducting, whereas the negative pulses will have no effect upon the tube 250. There will thus be an impulse impressed upon the tube 250 once for each cycle and the impulse may be accurately oriented with respect to the start transition by means of the potentiometers 242 and 243 and is usually oriented to occur slightly before the center of each standard pulse period, notas established ln the line circuit under test, but as established by the slightly delayed operations of relays and i60, for control of the unit condensers IBI and IGI.

Condenser timing circuit The condenser timing circuit, including the gas-filled tubes 250 and `260, is provided to substantially' instantaneously discharge one or the other of the unit condensers I'5I and IBI, whichever happens to be connected to the constant current circuit 336-336a at the middle of each pulse v period after relay |10 has been operated to spaccondenser I8 I.

ing at the arrival of a Start transition.

The circuits for the gas-filled tube 250 may be traced as follows. The cathode is connected over conductor 253, spacing contact of relay |10 to the negative constant current conductor 33Go to which is also connected, say, the grounded unit The plate circuit is connected to ground through lnductance 256 and resistance 251. The control grid is connected over resistance 22, the secondary winding .of transformer 24| directly to the negative constant current con-f ductor 336. Thus, with no voltage impulse present in the secondary f transformer 24|, the grid of tube 250 receives a negative potential relative to the cathode which is equal to the potential drop in resistance 21|) of 15 Volts due to the constant current iiowing into unit condenser |6| and under this condition the gas-filled tube remains non-conducting. However, when a positive Voltage impulse of, say, 60 volts from transformer 24| is impressed on the grid of tube 250, the tube becomes ionized and thus establishes an oscillatory discharging circuit from the grounded negatively charged condenser through the tube and the inductance 256 and resistance 251 to ground. The condenser now quickly discharges and, due to the inductance 256, tends to charge in the positive direction.

As will appear from the detailed description below of the operation of the system the magnitude of the negative voltage on condenser |6|, taken as an example, at the time it begins to discharge through' the tube 250, depends on the arrival time of the last preceding transition. If, therefore,

the condenser current were permitted to flow through the tube to charge the condenser in the positive direction, the tube would not be extinguished and' the recharging of the condenser could not begin until the instant the current attained zero value; the positive condenser potential at this instant being nearly equal to the initial negative potential, it too would depend on the arrival time of the last transition. However,

since the recharging of the condenser to negative potential is utilized for comparison purposes relating to the arrival time of the next transition, it must be made independent of any previous transition. This is attained by means of the circuit including the gas-filled tube 260.

The circuit for the gas-filled tube 260 may be traced as follows. The plate is connected through resistance 261 to positive battery and is also connected through a normally charged condenser 255 to the plate circuit of tube 250 and the oscillatorydcircuit just described. The cathode is connected to ground. The control grid is connected through resistance 265 to the constant current conductor 336e and thus normally receives a negative potential, thereby maintaining the tube 260 non-conducting. During the oscillatory discharge of condenser |6| through inductance 256, described above, the negative potential on the grid of tube 26|) will quickly decrease with that of the constant current conductor 336a; when this potential passes through zero the tube 26D is fired, thereby lowering the positive potential of the lower side of condenser 255 to the sustaining plate potential of tube 26|) and thus forcing the upper side of condenser 255 and the plate of tube 250 sufficiently negative to extinguish the latter tube. This thus removes the discharge condition from condenser |6I, which now begins to charge to negative potential from the constant current conductor 336e. The ring of tube 260 establishes an oscillatory circuit comprising condenser 255 and inductance 256, and when the current in this circuit becomes zero, tube 260 is extinguished.

Y By this arrangement the current through condenser |6| is interrupted by the tube 250 at the instant the condenser potential reaches zero. The time interval between maximum and zero amplitude of potential in the oscillatory circuit being xed by the frequency of oscillation and i'll thus being independent of the maximum amplitude, the discharging time will be constant and the condenser will begin to recharge to negative from zero charge and at a predetermined instant, and thus independently of the previous transition. The charge and discharge of theunit condensers |5| and |6| under the control partly by the condenser timing circuit andv partly by the comparison circuit is illustrated in Figs. 5-I and 5-J, re-

spectively.

It will be noted that. when relay |10 opens its spacing contact at the beginning of the stop period, the cathode of tube 250 will be disconnected from the constant current conductor 336a. However, a permanent circuit is established from the cathode through the high resistance 212 to the constant current conductor to stabilize the potential of the cathode during the stop period and thus insure that the tube will remain extinguished.

By the circuit arrangements just described the discharge of the unit condensers may be completed in a very short time without exceeding the maximum permissible current in the discharge path. The current wave in this` path is nearly of the form of a half-cycle sine wave and the ratio of peak current to the total charge dissipated is comparatively low in a wave form of this type. If the condensers were discharged in a resistive circuit, as would be the case with a mechanical distributor or contact interrupter,

the current wave would be of exponential form,

in which the ratio of peak value of current tov total charge dissipated is very high. Thus the discharge of the unit condensers in the present system may be completed in a much shorter time than in the prior art systems. v

rThe condenser timing circuit has been found to operate satisfactorily with the following circuit constants:

Gas-filled tubes 250 and 260, manufactured by Western Electric Company.' Type 338A Condenser .001 microfarad Resistance 252 225,000 ohms Condenser 255 4 microfarads Inductance 256 18 henries Resistance 251 40 ohms Condenser 262 .0002 microfarad Resistance 255 400,000 ohms Resistance 210 1.000 ohms Condenser 21| 4 microfarads Resistance -212 100,000 ohms The potential drop over resistance 210 is about volts, and is normally applied in negative direction to the grid of tube 250. The impulses from transformer '24| reach about 60' volts applied in positive direction to tube 250, ring the tube.

With the condenser |5| or IGI of 5.4 microfarads in circuit with inductance 256 and resistance 251, the time for bringing the charge down through zero will be about .002 second, and the peak current through tube 250 and'inductance 256 will not exceed .6 ampere. assuming an initial condenser voltage of 165. With the circiut constants .listed above the discharge of the unit condensers will be completed within ten per cent of the dot period, making the unit condensers available for test purposes during ninety per cent of the marking or spacingr interval. respectively, and thereby permitting accurate measurements of distortions close to plus and4 minus forty-five per cent.

Power supply circuit The power supply circuit derives power from any conyenient source of alternating current Sill which may be. a commercial power supply system. The current from the source Sill passes through a transformer 35i and a full-wave rectiler tube 352 to the supply terminals SM and 3l5. An inductance fllt is serially included and condenser 3M is connected across this circuit to smooth the ripples in the output.

The reference voltage supply circuit includes the resistance 34? and the cathode-plate circuit of vacuum tube 3d@ forming a potentiometer which establishes the reference voltage at point 348. Under normal conditions the current consumption of this circuit is low. However, when a load is connected to conductor 3&2, variation of the potential of point 348 will be limited by the action of tube 34D. When, for example, the potential of point 348 tends to become more negative, the grid-cathode potential becomes less negative. This' in turn causes an increased flow of plate current, thereby causing the potential of point 348 to become less negative and thus compensating for the original tendency of this point. This action takes place at the instant one of the unit condensers lil, i6! is connected to point 348, for comparison purposes, charged to a higher negative potential than the reference potential; when vthe condenser potential is less negative than the reference'potential the tube action will be reversed. This arrangement, therefore, maintains a substantially constant reference voltage at the times the comparison between the reference voltage and the voltage of condenser |58 or IGI are made. Since the rate of change of potential drop versus current in the anode-cathode circuit of tube 340 is very low, this circuit may be looked upon as a battery of very low resistance which permits the unit condenser to be quickly l@ on the ammeter 335.

The stop-compensating` voltage and the reference potential may be checked on the meter 3S@ which is normally connected through key 35i to measure the stop-compensating voltage on conductor 322 and which, in the alternate position of key 38l, will be connected to the point 3&8 of the reference potential, replacing resistance 382 in this circuit to insure that the reference potential remain unaffected by operation oi key 331'.

The constant current circuit being designed to relays E50 and i60.

supply a constant current against a wide range of potential in its output circuit, its voltage tends to rise excessively when its output circuit 336 is opened, as happens during the travel time of To limit such excessive rise the voltage regulator 266 is connected to the constant current conductor 33Go.

The voltage-regulating devices connected to diierent points in the circuit to stabilize operations are of well-known construction and are .adapted to serve this purpose by their specific voltage-current characteristic. They are gaslled tubes with low current consumption at normal voltage, but they consume a quickly rising 35 current as the impressed voltage rises above the normal value. Devices of this type are manufactured by the Radio Corporation of America, Incorporated.

The regulator tube 266 is of type VR105-30 and is connected to conductor 336:1 to limit the potendischarged with a heavy current, which in turni4 vacuum tube 346 for the reference potential circuit 342. In this manner the current in tube 34E) may be controlled automatically to insure that the reference potential is equal to the stop-compensating voltage during the stop condition regardless of normal variations of the power supnly voltage.

f As already explained, the constant current is passed through potentiometer 32 only when relay |10 is in marking position, as during the stop interval. There are, therefore, two current conditions in potentiometer 320 which thus tend to react'upon the potential of point 323 in the resistance bridge. This would consequently also affect the reference potential, which depends on the grid potential in tube 340 derived from potentiometer 325. To practically eliminate these variations in potentials, and also to reduce the effect of power voltage variations, a voltage regulator tube 324 is connected from ground to point 323, the potential of which, therefore, remains constant within very narrow limits. A more detial of this conductor to about volts.

The regulator tube 324 is of type VR-30 and is connected across potentiometer 320 to stabilize the stop-compensating voltage.

The two regulator tubes 32'! are of the type VR105-30 and are serially connected across the cathode and the screen grid of tube 33@ to stabilize the constant current.

Normal operation The operation of the system in response to an incoming pulse series representing a character will now be described and reference will be made to the schematic illustration of the various operations shown in Figs. 5-A to 5-K.

It will be assumed that the signal series, as received with a slight uniform delay by relays i563 and I'Sll, has transitions such as illustrated at B of Fig. 5, namely, a start transition from marking to spacing, occurring' at the standard transition instant indicated by the vertical line l, transition I from spacing to marking and arriving ahead of the standard transition time indicated by the vertical line i; transition II from marking to spacing arriving late with respect to the standard transition instant 2 transition HI from spacing to marking and arriving late with respect to the standard transition instant 3; no transition 1V; transition V from marking to spacing concurring with the standard transition instant 5 and the stop transition from spacing to marking concurring with the standard transition instant 6.

In response to the start transition relay Ul operates to spacing, thereby operating relays 50 and l5@ to spacing.

Relay |50 removes the unit condenser ISI from the reference potential conductor 342s and connects it to the constant current conductor 336e. As shown in Fig. 5-I, the condenser begins to charge beyond the reference potential, indicated by the horizontal line i-i. Relay |60 removes condenser |6| from the stop-compensating voltage, applied to constant current conductor 336a over the marking contact of relay |10 during the stop condition, and connects it to the reference potential. These operations in response to a start transition do not affect the bias-meter |90 or the peak-voltmeter 310.

Relay |40, in operating to spacing, applies negative potential through potentiometer |42 and upper winding of relay |80 to the plate circuit of the tube 220 which, therefore, becomes currentless. Relay |80 operates to spacing by means of its lower biasing winding. In spacing position relay |80 operates relay |10 in a circuit from -20 volts on potentiometer 8| through upper winding of relay |10, conductor |83, resistance 22| to plus battery. Tube 225 becomes nonconducting and the character timing circuit is thereby conditioned for the slow discharge of condensers 222' and 222a through high resistance 223. A negative, slowly rising potential is thus applied to the grid of tube 220 as illustrated in Fig. 5E. It is evident that so long as the grid of tube 220 maintains the tube 220 in non-conducting condition the relay |80 cannot be operated in response to'operations to marking of relay |40 during the signal series.

Upon the opening of the marking contact of relay |80, a potential of -50 volts on potentiometer is removed from the oscillatory circuit of the impulse circuit which immediately commences its first oscillation in the positive direction without any interfering transients. When the oscillation has increased to a predetermined positive potential applied to the grid of vacuum tube 240, the cathode-anode path in this tube becomes conducting and remains conducting until the oscillation again decreases below this value, as shown in Fig. F. Thus, a slowly rising and quickly falling current pulse Vflows through the detector tube and the primary of transformer 24| as shown in Fig. 5G, thereby producing a small ineffective negative voltage impulse in the secondary of transformer 24| followed by a strong and very shortpositive voltage impulse, as shown in Fig. 5-H. By proper ad- Justment of the orienting potentiometers 242 and 243 to secure a proper relation between the cathode-grid potential and the cathode-anode potential of tube 240 the strong positive impulse in the secondary winding of transformer 24| may be oriented to occur exactly at the proper instant in relation to the center of each standard pulse period, as determined by the operations of relays |50 and |00 on distortion-free signals.

with the positive vonage from transformer 24| applied 'to the grid of tube 250 at the proper instant, this tube is fired and thereby connects the grounded inductance 250 over conductor l253, spacing contact oi?v relay |10, constant current conductor 330e and spacing contact of relay |50 to the unit condenser |5i, the charging of which thus `will be discontinued, as shown in Fig. 5I. Condenser |5i, which now is included in the osciliatory circuit with inductance 25B, quickly discharges to zero potential, at which time the zero potential is applied overconductor 336s to the grid oi' gas-filled tube 280, firing this tube. The tube 240. in reducing the potential applied to one i iibiiitiiiiiii thru.

side of the charged condenser 205 impresses a negative potential on the plate bf tube 250, thereby extinguishing this tube and thereby also permitting the condenser |5| to again charge at a constant rate as shown in Fig. 5-I. Tube 260 is subsequently extinguished by the oscillation through inductance 250 and condenser 255, as already described.

With the arrangement of the gas tubes 250 and 260, as described, the condenser |55 may be discharged and the tube 250 extinguished within a very short interval and with a comparatively small maximum current, thereby reserving a longer charging period for the condenser |5| than can be secured with rotating distributors or even with tuned relay timing circuits.4

This condition will now prevail until the transition I arrives, in response to which relay |40 is operated back to marking, causing relays |50` and |60 to operate back to marking, but leaving relays |10 and |80 in their. spacing positions.

Condenser |6| is now disconnected from the reference potential and connected to the constant current conductor 336a for charging, as shown in Fign5-J.

Condenser |5| is disconnected from the constant current conductor 336a, having been charged to a potential proportional to the duration of the preceding charging time. Thus, in the case of transition I arriving at the standard transition time |.the charge on condenser |5| would be such that its voltage would be equal to the reference potential at the marking contact of relay |50; however, since transition I arrives early, the voltage on condenser |5| is less negative than the reference potential, as shown in Fig. 5-I, and at the instant the marking contact of relay |50 closes an equaiizingcurrent will flow in circuits that will now be traced.

One `of these circuits includes the peak-voltmeter and-may be traced from condenser |5| through marking contact of relay |50, resistance |52 and condenser |53 in multiple, conductor 34211, resistance 34|, primary of transformer 344. conductor 342 to the reference potential at point 348. Thus, a current impulse will be induced in the secondary winding of transformer 344 through one of the rectiflers 35| and 352 and condenser 36|v to ground. The consequent potential on condenser 36| is applied to the tube 300 which thus sets up an unbalanced condition in the bridge circuit for the peak-voltmeter 310 which thus gives a deilection proportional to the current strength in transformer 344 and, therefore, proportional to the displacement of the marking transition I from the standard transition instant I.

`The equalizing current from condenser I 5| may be traced over another circuit from marking contact of relay |50 over break contact b of relay H8, through the bias-meter |30, resistance' I 8l, break contact c of relay .|i8, condenser |83 and resistance |82 in multiple and break contact dof relay ||8 to the reference potential on the conductor 442a.- The bias-meter |90, being highly damped by the large shunt condenser |92, will give integrated deflections for a succession oi equalizing impulses proportional to the average bias of the impulses being measured. This meter may be calibrated by adjustment oi' resistance IBI. In the present instant the meter will be deflected to indicate the marking bias of transition I.

ance 256 is connected over conductor 253, spacing contact of relay |10 and conductor 336a through marking contact of relay |60 to condenser |6|, which now quickly discharges, as shown in Fig. -J. When the potential of conductor 33Go reaches zero by the discharge of condenser |6| through inductance 256, the gas tube y260 is again ilred, thereby quickly extinguishing the gas tube 250 and subsequently extinguishing'itself by the discharging of condenser 255. When tube 250 becomes non-conducting, condenser |6| again charges up from the constant current conductor 333a until the arrival of the spacing transition II. i

When transition II arrives, relays |50 and |60 operate to spacing and condenser |5| now is connected for charging from the constant current conductor 336a and the charging of condenser |6| is discontinued. Since transition Il arrived late`with respect to the standard transition instant 2, the charge on condenser |6| is such that its potential is more negative than the reference potential. Therefore, when the marking contact of relay |60 closes, an equalizing currentv will flow between condenser |6| and the reference potential over the circuit from condenser |6|, marking contact of relay |60, break contact f of relay |8,vresistance |62 and condenser |63 in multiple over conductor 342a through transformer 344, and conductor 342 to the reference potential at point 348. The equalizing current through transformer 344 will now ailect the peakvoltmeter 310 in the same manner as described above for transition I, the deiiection of the meter needle being in the same direction as before; the equalizing current will be about the same as before, because.the transition II was displaced with respect to the transition instant 2 about as much as was transition I with respect to transition instant I.

At the same time bias-meter |90 is affected by the equalizing current through resistance |62 and condenser |63 in multiple over a circuit from the right side of resistance |62. break contact c of relay ||8, through resistance |93, meter |90, break contact b of relay ||8 through resistance |52 and condenser |53 in multiple to the left side of resistance |62, which is connected to the reference potential. 'Ihe bias meter will now be affected in the same direction as for the previous reading for transition I, thus indicating marking bias. l

The impulse circuit now enters its third cycle and near the middle of the standard dot period condenser |5| is again discharged by the flashing of tube 250 and connected to recharge from the constant current supply.

The charging now continues until the transition III arrives. As shown in Fig. 5--B this transition arrives later with respect to the standard transition instant 3 than did transition II with respect to' transition instant 2. Therefore, when relays 40, |50 and |60 operate toA marking, a greater equalizing current flows from condenser |5I. giving a higher reading on the peak-voltmeter 310 and deflecting the bias-meter |90 towards the side indicating spacing bias.

Condenser |6I now charges up to the reference it is discharged and then again charges at a constant rate.

With no transition IV, relays |40, |50 and E65 remain in marking position and condenser |6| continues to charge until the middle of the next dot period when it is again discharged and commences to recharge at a constant rate.

Transition V arrives on time so that, when relays |40, |50 and |60 operate to spacing, the condenser |=6| will be charged exactly to the reference potential and no equalizing current will ow. Due to the rectifying action of the tubes and 352 the charge on condenser 36| cannot be reduced when the equalizing current for a given transition is less than for a previous transition. Thus upon comparison of the transition V, the peak-voltmeter will continue to show the deection for transition III. The bias-meter S0, having received no impulse since transition III, tends towards a zero-bias reading. Condenser |5| now charges, discharges and recharges until the arrival of the stop" transition to marking. With this transition arriving on time, there will be no equalizing current.

During the reception of all these transitions the condensers 222 and 222a have been slowly discharging and have commenced to be charged in the opposite direction so that shortly after the standard transition instant 6, corresponding to the stop transition, the voltage on these condensers will be equal to the potential at point 226 supplied from potentiometer |8|. At this time the potential at point 221 passes through zero and tends to become positive thereby rendering the rectier tube 225 conducting and also conditioning the tube 220 for conduction. Point 21 thus is grounded through the rectiiler tube With the stop transition arriving on time relay |40 will have operated to marking at the time tube 220 is conditioned for conduction. With plus battery applied from the marking con-A tact of relay |40 to the plate circuit for tube 220, current flows through the tube and the upper winding of relay and operates this relay to marking, thereby disconnecting the negative potential at potentiometer |8| from point 226 so that condensers 222 and 222a will be quickly charged from battery over resistance 22| and through the rectier tube 225 to be ready for the next start transition, see Figs. 5-C, D and E.

At this time relay |10 is operated to marking by its lower biasing Winding, thereby again placing the stop-compensating voltage from conductor 322 upon the constant current conductor 335a and, therefore, upon condenser |6|. 'I'he constant current from tube 330 now ilowing through the potentiometer 320, the stop-compensating voltage applied to condenser |6| will be equal to the reference potential. Condenser |5| vremains connected to the reference potential.

The operation of relay |80 to marking also placed a negative potential of 50 volts from potentiometer |8| upon'the oscillating circuit for tube 230, and, due to the presence of the damping resistances 236'and 234, the oscillations are quickly restored to the steady state Within the duration of the stop impulse, even allowing for a late arrival of the "stop" transition. With no impulses from theimpulse circuit, the gas-filled tubes 250 and 260 thereafter remain' dormant. The bias-meter tends to subside toward a zero reading and the peak-voltmeter 310 mainpotential and near the center of 'the dot period 7l bains itspeak reading'. The entire test Circuit is,

rcllilerent diagrams.

therefore, restored to normal awaiting the arrival oi the next start transition.

When the stop" transition arrives early or late, there will, of course, be an equalizing cur-l rent between condenser 'I5I and the reference potential, which may affect both meters.

If the stop transition should arrive so late that the charge on condensers 2,22 has already reached the point where the grid potential of tube 220 has conditioned this tube for conduction, the character `timing circuit would await the operation to marking of relay I 40 in response to the stop transition, since tube 220 cannot conduct with negative potential applied to its plate from relay |40. Upon arrival of the stop transition the entire circuit would be restored to stop condition, as described above. 'There is thus no danger of the character timing circuit restoring the system to stop condition before the stop transition arrives, and it is insured that even a large displacement of the "stop" transition will be accurately indicated on the meters.

When the "stop" transition is greatly delayed, say with a forty per cent spacing bias, a special v condition arises. 'I'he operations of the system l under this assumed condition are indicated in Fig. by dotted lines in the stop interval of the All the operations will progress as before,V and the heavy equalizing current from condenser IIlI due to the delayed "stop transition will aiect the meters |90 and 310 as before. However, as the oscillatory circuit is returned to its steady-state condition by the operation of relay |80 to marking, an impulse may be produced in transformer 24|. Gas tube 250, which is now connected to conductor @36a only through resistance 212, since relay is operated to marking, will remain extinguished, reslstance 212 being oi such a high value that a discharge cannot be maintained. The condenser IBI, being connected to the stop-compensating potential remains charged. Thus, there will be no effect upon the meter readings after the stop" transition has been compared.

From the description of the operation, presented above, it will be apparent that the tube 250 is made conducting for six short intervals, as shown in Fig. 5-K, during which the unit condensers ISI or IBI are completely discharged. These conducting periods thus establish uniformly distributed reference instants which may be oriented to occur exactly at the 'center of each standard dot period. By charging cnc or the other condenser with the constant current after each reference instant, the exact arrival time ot the next transition may thus be determined quantitatively by means of the two meters.

It will be noted that the bias-meter |90 dur` by the space-to-mark transitions, is connected to the bias-meter in the marking position ci' relay |50 through a normally closed key M--S.l When this key is opened the charges of this condenser are prevented from affecting the meter reading which thus indicates the average displacement with respect to the "start" transition of all the mark-to-space transitions. Similarly, condenser I6I is connected over the spacingcontact on relay I00 through a normally closed key S-M to the other side of the meter circuit so that, when Alternative modes of operation The testing circuit, as already described, is, of course, suitable for operation on a seven-unit code, since even with maximum measurable distortion of the stop transition, the circuit is returned' to its original steady-state condition before the end of seven unit pulse lengths.

'I'he set may furthermore be adjusted for op.

eration with signals using 8 or 81/2 unit code of the same pulse frequency as the 7 or 'I1/2 unit code by operation of the key 201. This opens a short circuit for resistance 223a which thus ls inserted in series with resistance 223 in the slow set at other speeds.

discharge circuit for condensers 222. The discharge is thereby further retarded so that there will be time for a sixth selecting pulse before the arrival of the stop transition and the restoration of the test circuit to normal. The operations of the test set in response to the additional transition will be exactly the same as for the other transitions.

When key 201 is operated a warning signal is impressed on the lamp |00 from an interrupter or impulse generator 208, producing |20 impulses per minute, over key 201, conductor` IIB, make contacts c of relay |04 tothe lamp I 06, which will flicker. at a fast rate, thereby indicating at the test set appearances that the circuit is adjusted .to an abnormal condition. This signal.

is distinctly different iromgthe demand signal of 60 impulses per minute impressed at certain times upon this lamp through the interconnecting circuit, referred to above.

As already stated, the circuit is normally arrangedy for an operating speed of 23 cycles per second. Provision is also made for operating the For an operating speed of 28 cycles per second, key |01 is operated, thereby closing an operating circuit, over make contact.

d on relay |04, conductor II2, through a plurality of relays IIB, 20|, 202 and 203, thereby oper.. ating these relays.

The operation of relay II6 ,replaces the condensers IBI and IBI by condensers I5|a and llila, which are of smaller capacity to receive a standard charge corresponding to the same reference potential with the same constant current as before in a shorter time. corresponding to the speed oi about 28 cycles per second, or '15 words per minute with the 'I1/2 unit code and 66 words per minute with the `231/2 unit code. For a given time displacement of a signal transition relative to the corresponding standard transition instant, the difference between the condenser potential and the reference potential will 'be greater for these smaller condensers than beproportional to the 'change of speed it is not necessary to recalibrate meters and 310.

The operation oi relay 20| disconnects the condenser 222a from the character timing circuit so that the .time constant of this circuit will be changed to agree with the shorter internal between the start and stop transitions at the higher speed. The character timing circuit otherwise operates 1 as before.

The operation of relay 202 changes the tuning of the impulse circuit by replacing adjustable condenser 232 by adjustable condenser 232a over contacts d. The decrement potentiometer 233 is also replaced by potentiometer 23M over contacts b and c. Thus, the circuit for the tube 230 oscillates with a frequency corresponding to the standard frequency of about 28 cycles per second, and the decrement may be adjusted to maintain the amplitude of oscillation substantially constant during a complete pulse series representing a character. start circuit |82 is also changed at contacts a of relay 202 by the replacement of the resistance 234 by higher resistance 234e, to insure that the oscillator circuit, at the higher irequency, is returned to steady-state condition in a critically damped manner before the end of the signal train.

The operation of relay 203 replaces the orienting potentlometers 242 and 243 by potentiometers 24M/and l243a.V The impulses through transformer 24| may thus be oriented within the shorter cycle without disturbance of the orientation for the normal speed of 23 cycles per ,l

second.

In all other respects, theY circuit is arranged the same and operates in the same manner as described above.

When it is desired to measure signals transmitted at the speed of 15 cycles per second corresponding to 40 words per minute with the '1l/i unit code, the key |01 must be operated thereby' placing the circuit in the condition just described for the high speed. In addition, it is necessary to operate key 205, which adds relays ||1 and 204 to the relay-operating circuit ||2 from key |01.

The operation of relay ||1 connects the larger unit condensers |5|b and ilb into the comparison circuit replacing the other condensers.

The operation of relay 204 by its contact a, connects the condenser 222b in multiple to condenser 222 over a make contact on relay 20|. The character `timing circuit is thereby slowed up to' allow for the longer interval between the start and stop transitions. Relay 204, by its contact b, changes the frequency of the impulse circuit by adding the fixed condenser 232|) to the adjustable condenser 232a, thereby slowing up the frequencycf the oscillator tube 230 to correspond to the standard dot frequency of about cycles per second. The start circuit |02 from relay |80 for the oscillating circuit is changed by resistance 234a being short-circuited by contacts c of relay 204. It will, of course. be necessary to rea'djust condenser' 232e, potentiometer 233a and the orienting potentiometers 242m and 243a for recalibration of the set. Otherwise, the circuit remains the same land operates as already described.

The operation of key 206 now places a Warn-v ing signal 206 on the lamp |06 over make contact of relay conductor ||3a, key 201, conductor ||3 and make contacts c of relay |04 to the lamp |06. The signal produced by the signal generator 206 may be characteristically different from any other signals impressed upon lamp |06, but is preferably the same. as that The damping resistancein the generated by the device 2cd connected to the lamp by key 20F.

For operation of the test set with a commercial circuit using start-stop signals of the polar type, it is necessary to operate the key |619. This key operates relay thereby disconnecting the biasing winding o f relay so that this relay will be operated to marking or spacing in response to opposite directions of current in the line circuit through its upper winding. Otherwise, the test circuit operates as already described and may be set for the dilerent speeds as already described.

A reset key H0 is provided for discharging the condenser 36| in the peak-voltmeter circuit through the operation of relay 30|. This is for the purpose of dissipating the charge on condenser 36| and returning the meter 310 to zero reading before commencing each observation.

The set may be calibrated for any particular type of service by connecting it through the jack |03 to suitable circuits producing standard undisorted signals of the kind to be measured.

Certain features included in the system described above and illustrated in the drawings are being claimed in a copending application for patent Serial No. 432,823, nled on even date herewith, by W. T. Rea and J. R. Wilkerson.

What is claimed is:

l. A timing circuit of the relaxation oscillator type which comprises a timing condenser, a

source of direct current having a normal potential, rectifying means, relay means having contacts, a low resistance circuit connected between said source, said condenser and said rectifying means for quick charging of said condensei` to said potential in a given direction through said rectifying means in conducting condition, and a high resistance circuit connected between said source, said condenser an'd said contacts in closed condition for applying said normal potential in reverse direction to said condenser and to temporarily render said rectifying means non-conducting and initially establish a potential in sai'd high resistance circuit at least equal to twice said normal potential, thereby slowly changing theA charge on said condenser to a predetermined charge for restoring said rectifying means to conducting condition after a predetermined interval, said relay means being connected to be responsive to an incoming start pulse for closing said high resistance circuit and to be responsive to said predetermined charge for opening said high resistance circuit.

2. A timing circuit in accordance with claim i in which said source has a grounded point connected to said low resistance circuit for said lquick charging, and has points oi plus and minus potentials connected in said high resistance circuit to initially establish a potential therein greater than twice said normal potential and to cause a reversal of the `condenser charge during said slow changing of the charge for restoring said rectifying means to conducting condition at the end oiA said predetermined interval.

3. A timing circuit in accordance with claim 1 which further comprises a thermionic discharge tube having a control grid connected to said high resistance circuit for conditioning of said tube for conduction inresponse to said predetermined charge and having a plate circuit connected ior operating said relay means in the conducting condition of said tube to open said high resistance circuit.

andere 4. A timing circuit or cyclic operation com-Y prising a receiving relay having normally open contacts and connected to be responsive to successive incoming start pulses for closing said contacts to initiate each cycle, a timing condenser, a source of direct current having a normal potential, a normally conducting rectier continuously connected to one side of said condenser, a low resistance circuit connected for passing a heavy current through said condenser and rectier in a given direction at the end of each cycle, a high resistance circuit connected for passing a light current in the opposite direction through said condenser over said contacts when closed in response to a start pulse to thereby initially render said rectiiler non-conducting and to gradually diminish and thereafter reverse the charge potential on said condenser for restoring the conducting condition of said rectifier after a predetermined interval from said start pulse, said relay being connected to alternately be responsive l -to said reversed charge potential after said interval for opening of said contacts and initiating said passing of heavy current. Y

5. A start-stop telegraph system comprising a pair of normally charged test condensers to be substantially instantaneously conditioned to have a predetermined charge once during each pulse period of an incoming telegraph signal, said system further comprising an impulse circuit for producing a series of impulses in isochronism with the normal pulse periods oi said signal, a gaseous discharge tube being normally non-conducting and having a control grid connected to receive said impulses for rendering said tube conducting, relay means responsive to the incoming telegraph pulses for connecting said test condensers alternately for conditioning by said tube in conducting condition during alternate signal pulses, and inductance means connected in series by said relay means with said test condenser being conditioned for establishing an oscillatory circuit therewith, said tube being adapted to become extinguished each time the voltage of the test condenser being conditioned attains a predetermined value.

6. A start-stop telegraph system in accordance with claim which further comprises circuit means including asecond gaseous discharge tube responsive to the changing voltage of the test condenser being conditioned in time to extinguish said nrst tube each time the voltage o! the test condenser attains said predetermined value.

7. A start-stop telegraph system comprising a. test condenser to be substantially instantaneously discharged during alternate pulses' of an incoming telegraph signal and at a preiixed reference instant during each pulse period, said system further comprising an impulse circuit for producing a series of impulses for establishing said reference instants, a gaseous discharge tube being normally non-conducting and having a control grid connected to receive said impulses for rendering said vtube conducting in lresponse to each impulse, relay means responsive tothe incoming telegraph pulses for connecting said test condenser for discharge by said tube at the next reference instant, and inductance means connected in series with said testfcondenser by said relay means for together with the discharging condenser establishing an oscillatory discharging circuit, said tube being adapted to become extinguished eachjime the voltage of the discharging test condenser tends to reverse during discharging.

8. A start-stop telegraph system in accordance with `claim '7 which further comprises circuit means including a normally charged auxiliary condenser and a. second gaseous discharge tube connected to become conducting in response to a predetermined voltage of the test condenser duringv discharging and connected to in conducting condition apply; through said auxiliary condenser an extinguishing potential'to said nrst tube each time the voltage ol.' thedischarging test condenser tends to reverse.A

9. A start-stop telegraph signal testing system comprising a receiving and measuring circuit which comprises a pair ot test condensers adapted to be charged at a predetermined rate alternately during corresponding alternate pulses of a telegraph signal and to be substantially instantaneously discharged alternately at prefixed reference instants o1' time within their periods ofv charging, a meter circuit adapted for measuring charges on said condensers alternately between said periods of charging,` a source of constant charging current, and polar relay means responsivato transitions between pulses oi' a signal for connecting said test condensers in alternations for said charging and measuring. said testing system further comprising yan impulse circuit for producing a series of impulses at said reference instants, a gaseous discharge tube having a normally non-conducting plate circuit continuously connected to said constant current source and having a control grid connected to receive said impulses for rendering said tube conducting at each of said instants for discharging ofthe test condenser which is connected to said constant current source by said relay means, and inductance means continuously connected to said plate circuit for together with the discharging test condenser establishing an oscillatory circuit to quickly reduce the condenser charge, vsaid tube being adapted to become extinguished each time the voltage of the discharging test condenser tends to reverse during discharging to establish said reference instants.

i 10. A start-stop telegraph-signal testing system in accordance Withclaim 9 which furthercomprises an auxiliary gaseous discharge tube having a 'normally non-conducting plate circuit including a source of direct current and also having a control grid continuously connected to said constant current source for rendering said auxiliary tube conducting when the voltage of the test condenser being discharged tends to become reversed and a normallycharged awdliary condenser connected between the ilrst' and second said plate circuits for together with said inductance means establishing a second oscillatory circuit for initially rendering the rst 1said plate circuit nonconducting in response to the said auxlliarytube becomingy conducting, and for subsequently automatically rendering the second said plate circuit non-conducting to permit recharging o! said auxiliary condenser.

11. A nrst normally non-conducting gaseous discharge tube, an oscillatory circuit normally in the steady state and including inductance, capacitance and a source of unidirectional potential for normally charging said capacitance and connected to apply a current sustaining potential to said tube. an impulse producing circuit connected to said tube to lire it in response to each impulse, and an extinguishing circuit for said first tube including a second normally non-conducting gaseous discharge tube, a source of 'unidirectional potential connected to apply a current sustaining potential to said second tube and a capacitance circuit connected between said first and second tubes to apply an extinguishing potential to said first tube in response to the firing of said second tube, said second tube being connected to said oscillatory circuit to be red in response to the discharge of said capacitance to about zero potential and being connected to said capacitance circuit to be extinguished by discharge of said capacitance circuit.

12. An interrupter circuit for establishing a series of conducting periods of equal duration, an impulse input circuit for said interrupter circuit for producing a series of evenly. spaced impulses for starting each of said conducting periods in response to said impulses, and an oscillatory output circuit for said interrupter circuit including frequency determining means of a xed cyclel for determining the duration of each of said conducting periods in response to said impulsesfsaid interrupter circuit including a rst and a second normally non-conducting gaseous'discharge tube each having a discharge sustaining potential applied thereto and a capacitance circuit connected between said tubes for extinguishing said first tube in response to the firing of said second tube and for subsequently automatically extinguishing said second tube. said oscillatory output circuit including frequency determining inductance and capacitance connected to start oscillating by -the ring of said rst tube in response to said impulses and connected to apply an oscillating potential to said second tube :for firing thereof at zero potential after a quarter of a cycle thereby terminating each of said conducting periods.

13. An interrupter circuit `for establishing a series of conducting periods of equal duration, a start-stop impulse input circuit for said interrupter circuit responsive to a start pulse for producing a predetermined number of evenly spaced substantially instantaneous impulses for initiation of each of said conducting periods, and an oscillatory output circuit [for said interrupter circuit including frequency determining me' s of a fixed cycle/for discontinuing each o'fgsaid conducting periods after -a predetermifndduration in response to said impulses, said interrupter circuit .including a first and a second normally nonconducting gaseous discharge tube each having .a discharge sustaining potential applied thereto and a capacitance circuit connected between said tubes for extinguishing'said iirst tube in response to the firing of said/'second tube and for subsequently automatically extinguishing said second tube, said oscillatory output circuit including frequency deter/mining inductance and capacitance connected toV start oscillating by the ring of said rst tube in response to said impulses and connected to apply an oscillating potential to said second tube for firing thereof at zero potential after a quarter of a cycle thereby terminating each of said conducting periods, and said capacitance circuit being connected to said inductance to form a second oscillatory circuit therewith for reducing the discharge current in said second tube to zero after a predetermined time between successive conducting periods.

JEFFERSON R. WILKERSON. 

